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Search: Author = S.Harar

Found 37 matches.

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1998BE14      Phys.Rev. C57, 1788 (1998)

E.Berthoumieux, E.C.Pollacco, C.Volant, B.Berthier, Y.Cassagnou, J.L.Charvet, M.Colonna, R.Dayras, R.Legrain, C.Mazur, E.De Filippo, A.Cunsolo, A.Foti, G.Lanzano, A.Pagano, S.Urso, Sl.Cavallaro, R.Barth, V.Lips, H.Oeschler, S.Harar, E.Norbeck

Heavy Fragment Production in 40Ar + 232Th Reactions at 27A, 44A, and 77A MeV

NUCLEAR REACTIONS 232Th(40Ar, X), E=27, 44, 77 MeV/nucleon; measured light, intermediate, heavy fragments σ(E, θ); deduced fragment production mechanism.

doi: 10.1103/PhysRevC.57.1788
Citations: PlumX Metrics


1995PO05      Nucl.Phys. A583, 441c (1995)

E.C.Pollacco, E.Berthoumieux, E.De Filippo, C.Volant, R.Barth, B.Berthier, Y.Cassagnou, Sl.Cavallaro, J.L.Charvet, A.Cunsolo, M.Colonna, R.Dayras, D.Durand, A.Foti, S.Harar, G.Lanzano, R.Legrain, V.Lips, C.Mazur, E.Norbeck, H.Oeschler, A.Pagano, S.Urso

Production of Heavy Fragments in the Reaction 40Ar + 232Th

NUCLEAR REACTIONS 232Th(40Ar, X), (40Ar, F), E=44, 77 MeV/nucleon; measured fission, other fragment velocity vs mass, singles, coincidence modes; deduced heavy fragment production mechanism. Boltzmann-Nordheim-Vlasov approach.

doi: 10.1016/0375-9474(94)00701-N
Citations: PlumX Metrics


1994LI03      Phys.Rev. C49, 1214 (1994)

V.Lips, R.Barth, G.Klotz-Engmann, H.Oeschler, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, R.Legrain, E.C.Pollacco, C.Volant

Deep Inelastic Collisions in the System 40Ar + 232Th at 31 MeV/nucleon

NUCLEAR REACTIONS 232Th(40Ar, X), E=31 MeV/nucleon; measured fragment σ(θ, Z) vs velocity; deduced total kinentic energy loss, projectile fragment σ(θ).

doi: 10.1103/PhysRevC.49.1214
Citations: PlumX Metrics


1993PO12      Z.Phys. A346, 63 (1993)

E.C.Pollacco, C.Volant, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, R.Legrain, J.-E.Sauvestre

Fission Study for the System 84Kr + 232Th at 25, 35 and 45 MeV/u

NUCLEAR REACTIONS 232Th(84Kr, F), E=25-45 MeV/nucleon; measured fission (fragment)(fragment)(θ); deduced heavy residue recoil velocities, target plus projectile fusion evidence.

doi: 10.1007/BF01290782
Citations: PlumX Metrics


1993YE01      Phys.Rev. C48, 1092 (1993)

S.J.Yennello, K.Kwiatkowski, E.C.Pollacco, C.Volant, Y.Cassagnou, R.Dayras, D.E.Fields, S.Harar, E.Hourani, R.Legrain, E.Norbeck, R.Planeta, J.L.Wile, N.R.Yoder, V.E.Viola

Studies of Intermediate-Mass Fragment Emission in the 3He + (nat)Ag, 197Au Reactions between 0.48 and 3.6 GeV

NUCLEAR REACTIONS Ag, 197Au(3He, X), E=0.48-3.6 GeV; measured σ(fragment θ, E) for fragment Z=4-9; deduced energy dissipation, emitting source expansion features. Models comparison.

doi: 10.1103/PhysRevC.48.1092
Citations: PlumX Metrics


1990PO10      Nucl.Phys. A519, 197c (1990)

E.C.Pollacco, C.Volant, R.Dayras, Y.Cassagnou, S.Harar, R.Legrain, C.Mazur, S.J.Yennello, K.Kwiatkowski, N.R.Yoder, V.E.Viola, R.Planeta, J.L.Wile, D.E.Fields, E.Hourani, E.Norbeck

Search for the Onset of Multifragmentation in the Reaction 3He + (nat)Ag

NUCLEAR REACTIONS Ag(3He, X), E=0.48-3.6 GeV; measured σ(fragment θ, E).

doi: 10.1016/0375-9474(90)90626-W
Citations: PlumX Metrics


1990YE05      Phys.Lett. 246B, 26 (1990)

S.J.Yennello, K.Kwiatkowski, D.E.Fields, R.Planeta, V.E.Viola, Jr., E.C.Pollacco, C.Volant, R.Dayras, R.Legrain, Y.Cassagnou, S.Harar, E.Hourani

Complex Fragment Emission from the 3He + (nat)Ag System between 0.48 and 3.6 GeV

NUCLEAR REACTIONS Ag(3He, X), E=0.48-3.6 GeV; measured σ(fragment θ, E); deduced reaction mechanisms energy dependence.

doi: 10.1016/0370-2693(90)91302-R
Citations: PlumX Metrics


1989KL01      Nucl.Phys. A499, 392 (1989)

G.Klotz-Engmann, H.Oeschler, J.Stroth, E.Kankeleit, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, R.Legrain, E.C.Pollacco, C.Volant

Properties of Binary Fission and Multifragmentation in the Transition Regime

NUCLEAR REACTIONS 232Th(α, F), (14N, F), E=250, 800 MeV/nucleon; 197Au, 165Ho(α, F), E=70, 250, 800 MeV/nucleon; Ag(α, F), E=800 MeV/nucleon; 197Au(14N, F), E=250 MeV/nucleon; measured fission σ, (fragment)(fragment)(θ), fragment velocities, fragment energy.

doi: 10.1016/0375-9474(89)90054-7
Citations: PlumX Metrics


1987HA28      Nucl.Phys. A471, 205c (1987)

S.Harar

Entrance Channel Influence on the Formation and Decay of Hot Nuclei

NUCLEAR REACTIONS, MECPD 232Th(58Ni, X), E=20, 25, 30 MeV/nucleon; 232Th(40Ar, X), E=31, 35, 39, 44 MeV/nucleon; 232Th, 165Ho(14N, X), E=60 MeV/nucleon; 165Ho(40Ar, X), E=31, 44 MeV/nucleon; measured fusion fragment σ(θ1, θ2); deduced entrance channel role, hot nuclei formation, decay mechanisms.

doi: 10.1016/0375-9474(87)90252-1
Citations: PlumX Metrics


1987KL02      Phys.Lett. 187B, 245 (1987)

G.Klotz-Engmann, H.Oeschler, E.Kankeleit, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, M.Mostefai, R.Legrain, E.C.Pollacco, C.Volant

Transition From Fission to Multifragmentation

NUCLEAR REACTIONS Ag, 165Ho, 197Au(α, X), E=70-800 MeV/nucleon; measured fragment mass spectra, relative velocities; deduced fission, multi-fragmentation characteristics. Tof telescopes.

doi: 10.1016/0370-2693(87)91089-6
Citations: PlumX Metrics


1987VO07      Phys.Lett. 195B, 22 (1987)

C.Volant, M.Conjeaud, S.Harar, M.Mostefai, E.C.Pollacco, Y.Cassagnou, R.Dayras, R.Legrain, G.Klotz-Engmann, H.Oeschler

Formation and Decay of Hot Nuclei

NUCLEAR REACTIONS 232Th(58Ni, X), E=20, 25, 30 MeV/nucleon; measured (fragment)(fragment)-coin, σ(E), σ(E, θ1, θ2); deduced reaction mechanism. Exciton model calculations.

doi: 10.1016/0370-2693(87)90879-3
Citations: PlumX Metrics


1985CO19      Phys.Lett. 159B, 244 (1985)

M.Conjeaud, S.Harar, M.Mostefai, E.C.Pollacco, C.Volant, Y.Cassagnou, R.Dayras, R.Legrain, H.Oeschler, F.Saint-Laurent

Central Collisions in the Argon Induced Fission of Thorium in the Transition Energy Regime

NUCLEAR REACTIONS 232Th(40Ar, F), E=31, 35, 44 MeV/nucleon; measured fission fragment σ(θ1, θ2), energies, masses, velocities; deduced collision energy dependence, large, small momentum transfer reaction σ(E).

doi: 10.1016/0370-2693(85)90243-6
Citations: PlumX Metrics


1984PO14      Phys.Lett. 146B, 29 (1984)

E.C.Pollacco, M.Conjeaud, S.Harar, C.Volant, Y.Cassagnou, R.Dayras, R.Legrain, M.S.Nguyen, H.Oeschler, F.Saint-Laurent

High Momentum and Energy Transfer Induced by 1760 MeV 40Ar on 197Au and 232Th Targets

NUCLEAR REACTIONS 197Au, 232Th(40Ar, F), E=1760 MeV; measured fission (fragment)(fragment)(θ), masses, velocities, energies; deduced mass transfer process dominance.

doi: 10.1016/0370-2693(84)90636-1
Citations: PlumX Metrics


1984SA15      Nucl.Phys. A422, 307 (1984)

F.Saint-Laurent, M.Conjeaud, R.Dayras, S.Harar, H.Oeschler, C.Volant

Momentum Transfer in Light-Ion-Induced Fission Reactions

NUCLEAR REACTIONS, ICPND 232Th(p, F), E=140-1000 MeV; 232Th(d, F), E=70-1000 MeV; 232Th(α, F), E=280, 1000 MeV; 197Au(α, F), E=280 MeV; measured fission σ, σ(fragment θ), (fragment)(fragment)(θ). 233,234Pu, 236U deduced spins, linear momentum transfer. Intranuclear cascade model.

doi: 10.1016/0375-9474(84)90519-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0647.


1982SA08      Phys.Lett. 110B, 372 (1982)

F.Saint Laurent, M.Conjeaud, R.Dayras, S.Harar, H.Oeschler, C.Volant

Momentum Transfer with Light Ions at Energies from 70 MeV to 1000 MeV

NUCLEAR REACTIONS, Fission 232Th(p, F), E=140, 250, 500, 1000 MeV; 232Th(d, F), E=70, 140, 500, 1000 MeV; 232Th(α, F), E=69.2, 140, 280, 1000 MeV; measured (fragment)(fragment)(θ); deduced dominating processes, corresponding regions. 233,234Pa, 236U deduced forward momentum transfer during fission.

doi: 10.1016/0370-2693(82)91275-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0011.


1980WI09      Phys.Lett. 93B, 35 (1980)

J.P.Wieleczko, S.Harar, M.Conjeaud, F.Saint-Laurent

Entrance Channel Versus Compound Nucleus Limitations in the Fusion Process of 1p and 2s-1d Shell Nuclei

NUCLEAR REACTIONS 12C(14N, X), 10B, 12C, 16O(17O, X), E(cm)=12-30 MeV; measured fusion σ(E); deduced entrance channel, compound nucleus effects.

doi: 10.1016/0370-2693(80)90089-1
Citations: PlumX Metrics


1979SA26      Nucl.Phys. A327, 517 (1979)

F.Saint-Laurent, M.Conjeaud, S.Harar, J.M.Loiseaux, J.Menet, J.B.Viano

Formation and Deexcitation of the 32S Compound Nucleus via the 20Ne + 12C and 16O + 16O Entrance Channels

NUCLEAR REACTIONS 12C(20Ne, X), E=67.1, 81, 92.3, 135, 157 MeV; 16O(16O, X), E=119, 141 MeV; measured σ for residual elements with Z=5-15; deduced limiting angular momenta for fusion, reaction mechanism.

doi: 10.1016/0375-9474(79)90272-0
Citations: PlumX Metrics


1978CO20      Nucl.Phys. A309, 515 (1978)

M.Conjeaud, S.Gary, S.Harar, J.P.Wieleczko

Complete Fusion of the 12C + 12C, 14N + 12C and 15N + 12C Systems

NUCLEAR REACTIONS 12C(12C, X), 12C(14N, X), 12C(15N, X), E=27-60 MeV; measured σ for residual elements for Z=6-13; deduced limiting angular momenta for fusion. Statistical model analysis of evaporation residues cross sections. Entrance, compound nucleus effects discussed.

doi: 10.1016/0375-9474(78)90493-1
Citations: PlumX Metrics


1977LE17      Nucl.Phys. A289, 187 (1977)

A.Lepine, C.Volant, M.Conjeaud, S.Harar, E.F.da Silveira

16O Induced Reactions on 116Sn at 64 MeV

NUCLEAR REACTIONS 116Sn(16O, 16O), (16O, 16O'), (16O, 15N), (16O, 14C), E=64 MeV; measured σ(θ); deduced deformation, optical model parameters. 117Sb, 118Te levels deduced S. DWBA, CCBA analysis.

doi: 10.1016/0375-9474(77)90528-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0991.


1977VO08      J.Phys.(Paris) 38, 1179 (1977)

C.Volant, M.Conjeaud, S.Harar, E.F.da Silveira

Compound Nucleus Formation in the 14N + 16O System

NUCLEAR REACTIONS 16O(14N, X), E=20-60 MeV; measured σ(E).

doi: 10.1051/jphys:0197700380100117900
Citations: PlumX Metrics


1975CO15      Nucl.Phys. A250, 182 (1975)

M.Conjeaud, S.Harar, E.F.Da Silveira, C.Volant

Transfer Reactions Induced by 12C on 18O and 26Mg at 46 MeV

NUCLEAR REACTIONS 18O(12C, 10Be), 26Mg(12C, 11B), (12C, 10Be), (12C, 9Be), E=46 MeV; measured σ(θ). 26Mg(12C, 12C) deduced optical model parameters. 20Ne, 27Al, 28Si, 29Si levels deduced S. DWBA analysis with microscopic, cluster form factors. Enriched targets.

doi: 10.1016/0375-9474(75)90208-0
Citations: PlumX Metrics


1975CO25      J.Phys.(Paris), Colloq. 36, C5-111 (1975)

M.Conjeaud, S.Harar, A.Lepine, E.Da Silveira, C.Volant

Etude de Reactions Induites par des Projectiles 16O sur Une Cible 116Sn a 64 MeV

NUCLEAR REACTIONS 116Sn(16O, 16O), (16O, 16O'), (16O, 15N), (16O, 14C), E=64 MeV; measured σ(θ); deduced optical model parameters.


1975VO02      Nucl.Phys. A238, 120 (1975)

C.Volant, M.Conjeaud, S.Harar, S.M.Lee, A.Lepine, E.F.Da Silveira

Evidence for Critical Angular Momenta in the Formation of 26Al via the 14N + 12C Channel

NUCLEAR REACTIONS 12C(14N, 6Li), E=20-60 MeV, measured σ(E;θ); 12C(14N, d), E=20-40 MeV, measured σ(E), σ(θ); 20Ne, 24Mg deduced levels.Hauser-Feshbach calculations, suggested critical angular momenta for the 26Al compound nucleus formation.

doi: 10.1016/0375-9474(75)90343-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0504.


1973CO33      Nucl.Phys. A215, 383 (1973)

M.Conjeaud, S.Harar, M.Caballero, N.Cindro

The (t, α) Reaction on Even Tellurium Nuclei

NUCLEAR REACTIONS 122,124,126,128Te(t, α), E=12 MeV; measured σ(Eα, θ). 121,123,125,127,129Sb deduced levels, L(p), π, J, S. Enriched targets.

doi: 10.1016/0375-9474(73)90662-3
Citations: PlumX Metrics


1972CA41      An.Fis. 68, 155 (1972)

C.Caballero, J.Casanova, S.Harar

Estudio de la Estructura de los Isotopos del Sb Mediante las Reacciones A52(t, α)A-151Sb y A-Te(t, t)A-Te

NUCLEAR REACTIONS 122,124,126,128,130Te(t, α);E=11.8 MeV; measured σ(Eα, θ); 126Te(t, t);E=11.8 MeV; measured σ(θ). 121,123,125,127,129Sb deduced levels.


1972HA09      Nucl.Phys. A183, 161 (1972)

S.Harar, R.N.Horoshko

Study of the Level Scheme of 117In via Proton Transfer Reactions

NUCLEAR REACTIONS 116Cd(3He, d), E=27 MeV; 116Cd(α, t), E=25.5 MeV; measured σ(Ed, θ), σ(Et). 117In deduced levels, J, π, L(p), S. Enriched 116Cd target.

doi: 10.1016/0375-9474(72)90936-0
Citations: PlumX Metrics


1972PA16      Phys.Rev. C5, 1995 (1972)

A.D.Panagiotou, H.E.Gove, S.Harar

High-Spin States in 20Ne and their Possible Classification into Rotational Bands

NUCLEAR REACTIONS 12C(12C, α);E=50, 51 MeV; measured αα(θ). 20Ne levels deduced J, π, γ-branching.

doi: 10.1103/PhysRevC.5.1995
Citations: PlumX Metrics


1969CO03      Nucl.Phys. A129, 10 (1969)

M.Conjeaud, S.Harar, E.Thuriere

Reaction (d, 3He) sur les Isotopes Doublement Pair de l'Etain

NUCLEAR REACTIONS 112,114,116,118,120,122Sn(d, 3He), Ed=22 MeV; measured σ(E(3He), θ), Q. 111,113,115,117,119,121In deduced levels, J, π, L(p), S. Enriched targets.

doi: 10.1016/0375-9474(69)90905-1
Citations: PlumX Metrics


1968BA56      J.Phys.(Paris), Suppl.No.1, Colloq.C1-162 (1968)

G.Bassani, M.Conjeaud, S.Harar, J.Picard, G.Souchere

La Reaction (tau, d) sur les Noyaux 88Sr, 90Zr et 92Mo

NUCLEAR REACTIONS 88Sr, 90Zr, 92Mo(3He, d), E=18 MeV; measured σ(θ). 89Y, 91Nb, 93Tc deduced levels, L(p), S.


1968BA57      J.Phys.(Paris), Suppl.No.1, Colloq.C1-163 (1968)

G.Bassani, M.Conjeaud, S.Harar, J.Picard, G.Souchere

Etats de Trou de Neutron dans les Noyaux N = 50

NUCLEAR REACTIONS 88Sr, 90Zr, 92Mo(3He, α), E=18 MeV; measured σ(Eα, θ). 87Sr, 89Zr, 91Mo deduced levels, L(n), S.


1968BI15      J.Phys.(Paris), Suppl.No.1, Colloq.C1-168 (1968)

L.Bianchi, M.Conjeaud, S.Harar, J.Picard, C.Ellegaard, P.Vedelsby

Reactions 115,113In(3He, d)116,114Sn

NUCLEAR REACTIONS 113,115In(3He, d), E=18 MeV; measured σ(Ed). 114,116Sn deduced levels.


1968CO22      Nucl.Phys. A117, 449 (1968)

M.Conjeaud, S.Harar, Y.Cassagnou

(3He, d) Reactions on the Even Tin Isotopes

NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(3He, d), E=18 MeV; measured σ(Ed, θ), Q. 113,115,117,119,121,123,125Sb deduced levels, J, π, L(p), S. Enriched targets.

doi: 10.1016/0375-9474(68)90855-5
Citations: PlumX Metrics


1966BA25      Phys.Letters 22, 189 (1966)

G.Bassani, M.Conjeaud, J.Gastebois, S.Harar, J.M.Laget, J.Picard, Y.Cassagnou

(3He, d) Reactions on the Even Sn Isotopes

NUCLEAR STRUCTURE 121Sb, 123Sb, 125Sb, 117Sb, 113Sb, 119Sb, 115Sb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90569-5
Citations: PlumX Metrics


1966CO25      Phys.Letters 23, 104 (1966)

M.Conjeaud, S.Harar, J.Picard

A Possible Process for Core Excitation in Even Single Closed Shell Nuclei

NUCLEAR STRUCTURE 116Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90144-2
Citations: PlumX Metrics


1966CO35      CEA-N-621, p.10 (1966)

M.Conjeaud, B.Fernandez, S.Harar, J.Picard, G.Souchere

Reactions (d, p) et (d, t) sur les Isotopes Pairs de l'Etain

NUCLEAR STRUCTURE 111Sn, 113Sn, 115Sn; measured not abstracted; deduced nuclear properties.


1965CO03      Nucl.Phys. 62, 225 (1965)

M.Conjeaud, B.Fernandez, S.Harar, J.Picard, G.Souchere

Diffusion de Neutrons de 14.6 MeV by le Soufre

NUCLEAR REACTIONS 32S(n, n), (n, n'), E=14.6 MeV; measured σ(En', θ). 32S deduced levels. Natural target.

doi: 10.1016/0029-5582(65)90865-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21101.


1963SO05      J.Phys. 24, 822 (1963)

G.Souchere, S.Harar, B.Fernandez, J.Picard, M.Conjeaud

Diffusion Inelastique de Neutrons de 14 MeV sur le Soufre 32

NUCLEAR STRUCTURE 32S; measured not abstracted; deduced nuclear properties.

doi: 10.1051/jphys:019630024011082201
Citations: PlumX Metrics


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